The expected abundance of Lyman-$α$ emitting primeval galaxies. I. General model predictions

Details The expected abundance of Lyman-$α$ emitting primeval galaxies. I. General model predictions The expected abundance of Lyman-$α$ emitting primeval galaxies. I. General model predictions

2003-12-14

arxiv.org/abs/astro-ph/0312363v2

Astronomy and Astrophysics

Astrophysics

18 pages, 12 figures, submitted to Astronomy & Astrophysics

Scientific paper

We present model calculations for the expected surface density of Ly-$\alpha$ emitting primeval galaxies (PGs) at high redshifts. We assume that elliptical galaxies and bulges of spiral galaxies (= spheroids) formed early in the universe and that the Ly-$\alpha$ emitting PGs are these spheroids during their first burst of star formation at high redshift. One of the main assumptions of the models is that the Ly-$\alpha$ bright phase of this first starburst in the spheroids is confined to a short period after its onset due to rapid formation of dust. The models do not only explain the failure of early surveys for Ly-$\alpha $ emitting PGs but are also consistent with the limits of new surveys (e.g. the Calar Alto Deep Imaging Survey - CADIS). At faint detection limits $S_{lim} \le 10^{-20}$W/m$^2$ the surface density of Ly-$\alpha$ emitters is expected to vary only weakly in the redshift range between $z=3$ and $z=6$ with values $> 10^3 / {deg}^2 / \Delta z = 0.1 $ reaching its maximum at $z_0 \approx 4$. At shallower detection limits, $S_{lim} \ge 3\times 10^{-20}$W/m$^2$ the surface density of high-z Ly-$\alpha$ emitters is expected to be a steep function of redshift and detection limit. This explains the low success in finding bright Ly-$\alpha$ galaxies at $z > 5$. We demonstrate how the observed surface densities of Ly-$\alpha $ emitting PGs derived from recent surveys constrain the parameters of our models. Finally, we discuss the possibility that two Ly-$\alpha$ bright phases occur in the formation process of galaxies: An initial -- primeval -- phase in which dust is virtually non-existing, and a secondary later phase in which strong galactic winds as observed in some Lyman break galaxies facilitate the escape of Ly-$\alpha $ photons after dust has already been formed.

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